Enhanced detection sensitivity with piezoelectric microcantilever sensors

ABSTRACT

A method for enhancing the detection sensitivity of a piezoelectric microcantilever sensor. The method may involve providing a piezoelectric microcantilever and inducing a change in the Young&#39;s modulus during detection of a species of interest. The change in the Young&#39;s modulus may be induced or enhanced by the application of a DC bias electric field to the piezoelectric layer that enhances non-180° polarization domain switching of the piezoelectric layer. The change in the Young&#39;s modulus may also result from binding of the species of interest to the piezoelectric microcantilever sensor or a combination of binding and application of a DC bias electric field Significantly enhanced detection sensitivity results from the changed Young&#39;s modulus of the piezoelectric layer.

STATEMENT OF GOVERNMENT INTEREST

This invention was reduced to practice with Government support under Grant No. RO1 EB000720 awarded by the National Institutes of Health; the Government is therefore entitled to certain rights to this invention. Some research for this invention was supported by the Commonwealth of Pennsylvania's Ben Franklin Technology Development Authority through the Ben Franklin Technology Partners of Southeastern Pennsylvania as fiscal agents for the Nanotechnology Institute.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The invention relates to methods and systems for enhancing the detection sensitivity of piezoelectric microcantilevers. The method of the present invention may be particularly beneficial for biodefense, food safety, pathogen detection and diagnostic applications involving body fluids such as serum, saliva, and urine.

2. Description of the Related Technology

Piezoelectric sensor technologies, specifically piezoelectric cantilever sensors, are useful for detecting the presence and/or mass of various compounds and molecules. Typically millimeter-sized, these cantilever sensors are fabricated by bonding a thick layer of a piezoelectric material, such as commercial lead zirconate titanate (PZT), to a non-piezoelectric substrate, such as stainless steel, titanium or glass, and have a number of advantageous properties, such as the capability of electrical self-excitation and self-sensing. Furthermore, piezoelectric cantilevers that include an insulation layer are capable of preventing conduction in liquid media, rendering them promising for biological in-situ electrical detection. Current piezoelectric cantilever sensors, however, generally lack the desired detection sensitivity necessary for many applications, particularly in-situ biosensing applications. These sensors typically have poor piezoelectric properties, characterized by a low −d₃₁ piezoelectric coefficient of less than 20 pm/v.

The detection sensitivity of piezoelectric cantilever sensors, which may be viewed as simple harmonic oscillators, is correlated to the resonance frequency shift capability of the sensor. The resonance frequency shift capability in turn is dependent upon the ability to detect changes in the effective spring constant and effective mass of the sensor. Current cantilever sensor technologies, such as non-piezoelectric microcantilevers and piezoelectric microcantilevers constructed from bulk PZT of relatively large thickness are only useful for methods which detect changes in mass and/or minor changes in the effective spring constant of the sensor.

Enhancement of detection sensitivity, accuracy and efficiency of piezoelectric cantilever sensors would be useful to the development of numerous industries and technological fields, such as bioterrorism defense, health sciences and diagnostic devices. Therefore, there is a need to develop a piezoelectric microcantilever sensor capable of achieving very high detection sensitivities.

SUMMARY OF THE INVENTION

In one aspect, the present invention is directed to methods for enhancing detection sensitivity of a piezoelectric microcantilever sensor. One such method involves providing a piezoelectric microcantilever sensor, applying a DC bias electric field to the sensor.

In another aspect, the method involves providing a piezoelectric microcantilever sensor wherein binding of the species of interest to the sensor induces a significant change in the Young's modulus of the piezoelectric layer.

In another aspect, the invention relates to a piezoelectric microcantilever sensor sensing system having enhanced detection sensitivity comprising a piezoelectric microcantilever sensor and a DC bias electric field generation means.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a cross-sectional view of one embodiment of a piezoelectric microcantilever in accordance with the present invention.

FIG. 2( a) is a flow cell system that can be used in conjunction with the cantilevers of the present invention.

FIG. 2( b) is a 3.5 in by 7.5 in portable PEMS sensor capable of working with 8 sensors and powered by a 9-V battery.

FIG. 3( a) is an optical micrograph of the PEMS.

FIG. 3( b) is a graph of phase angle as a function of the frequency flexural resonance spectrum.

FIG. 4( a) is a graph of phase angle as a function of the frequency resonance spectra at various RH with E=−4 kV/cm and

FIG. 4( b) is a graph of relative resonance frequency shift (Δf/f) versus relative humidity at E=−4, 0, and 4 kV/cm.

FIG. 5( a) is a graph of Δƒ(E)/ƒ as a function of E, where and ƒ and Δƒ(E) are the resonance frequency at zero DC bias electric field and the change of the resonance frequency at a DC bias electric field E relative to that without a DC bias electric field, respectively.

FIG. 5( b) is a graph of Δ∈(E)/∈ as a function of E, where ∈ and Δ∈(E) are the dielectric constant at zero DC bias electric field and the change of the dielectric constant at a DC bias electric field E relative to that without a DC bias electric field, respectively.

FIG. 6( a) is a graph of flexural-mode resonance spectra at 20% and 70% relative humidity. The insert figure is a top view of an optical micrograph of the PEMS.

FIG. 6( b) is a graph of (Δf/f)_(RH) and −d_(RH) as a function of relative humidity and (Δf/f)_(DC) and d_(DC) as a function of E of the PEMS. The insert figures show bending of the PEMS with an increasing E and a decreasing relative humidity, respectively.

FIG. 7 is a graph of (Δf/f)_(RH) as a function of relative humidity and (Δf/f)_(DC) as a function of E. The insert figures show a top view of an optical micrograph of the strip and a width-mode resonance spectra at 30% and 60% relative humidity.

FIG. 8 is a graph of Δƒ/ƒ and deduced ΔY_(p)/Y_(p) as a function of −∈_(ave) and −σ_(ave) for various relative humidity detection (solid circles) and various DC bias field measurements (solid squares), respectively.

FIG. 9 illustrates polarization domain switching.

FIG. 10 is a graph of Δf/f as a function of relative humidity under the influence of different DC bias electric fields.

FIG. 11 is a graph of Δf/f as a function of different DC bias electric fields, where Δf/f is the relative resonance frequency shift from 60% relative humidity (RH) to 30% RH.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

For illustrative purposes, the principles of the present invention are described by referencing various exemplary embodiments thereof. Although certain embodiments of the invention are specifically described herein, one of ordinary skill in the art will readily recognize that the same principles are equally applicable to, and can be employed in other apparatuses and methods. Before explaining the disclosed embodiments of the present invention in detail, it is to be understood that the invention is not limited in its application to the details of any particular embodiment shown. The terminology used herein is for the purpose of description and not of limitation. Further, although certain methods are described with reference to certain steps that are presented herein in certain order, in many instances, these steps may be performed in any order as may be appreciated by one skilled in the art, and the methods are not limited to the particular arrangement of steps disclosed herein.

It must be noted that as used herein and in the appended claims, the singular forms “a”, “an”, and “the” include plural references unless the context clearly dictates otherwise. Thus, for example, reference to “a sensor” includes a plurality of sensors and equivalents thereof known to those skilled in the art, and so forth. As well, the terms “a” (or “an”), “one or more” and “at least one” can be used interchangeably herein. It is also to be noted that the terms “comprising”, “including”, and “having” can be used interchangeably.

For purposes of the present invention, the terms “width mode”, “length mode” and “thickness mode” refer to various modes of use of the sensors for detection. Specifically, these modes refer to the direction of the induced stress relative to the cantilever sensor.

Additionally, for the purpose of this patent application, Q value is defined as the ratio of the resonance frequency to the resonance peak width at half the peak height.

The present invention pertains to various methods and systems for enhancing the detection sensitivity of cantilever sensors, particularly piezoelectric microcantilever sensors (PEMS) which use an electrical means for detection. Specifically, the method of the present invention involves providing a PEMS and using the PEMS to detect the presence or mass of a species of interest. It has been found that for certain PEMS sensors, a change in the Young's modulus of at least one piezoelectric layer of the PEMS sensor can be induced by the species of interest, thereby significantly enhancing the detection sensitivity of the sensor. The method of the present invention enables a PEMS to quickly, accurately and efficiently determine the presence and/or mass of a species of interest with a high level of detection sensitivity.

FIG. 1 shows the basic structure of a PEMS. The PEMS may include a first conductive element 1 and a second conductive element 2 (bottom electrode), a piezoelectric layer 7 located between the conductive elements 1, 2, receptors 5 located on said piezoelectric layer 7 and an optional receptor immobilization layer 4. For applications involving detection in, for example, liquid media, the PEMS may further include an electrically insulating layer 3 in order to increase tolerance of liquid damping or other environmental dampening.

In general, the effective mass and/or the effective spring constant of the piezoelectric layer change as a result of binding of a target species to the PEMS. By monitoring resonance frequency shifts which result from the mass and/or spring constant changes, the PEMS is capable of rapid, label-free, quantitative detection of various species, including pathogens, antigens, proteins, and DNA in a small volume of a sample medium (e.g. 100 μl) or in a cell culture using simple all-electrical measurements. The PEMS is capable of electric actuation and detection and may be used to create a PEMS array to enable simultaneous monitoring of multiple target compounds or molecules.

Conductive elements 1, 2 may be any element capable of conducting an electrical signal from the piezoelectric layer to a device for detecting that signal. In a preferred embodiment, conductive elements 1 and 2 are electrodes which may be constructed from any conductive material. Preferably, the first electrode 1 is constructed from Au/Cr or Pt/Ti and subsequently patterned in several regions. The second electrode 2 is preferably constructed from Pt/TiO₂ on SiO₂ for PZT/SiO₂ PEMS or Pt/Ti or Au/Cr on a metal substrate or non-piezoelectric layer. The electrode may be subsequently patterned.

Receptors 5 may be densely packed and immobilized onto, for example, any bi-functional linker modified sensor surface. Any receptor, such as specially synthesized cavitants, DNA oligonucleotides, proteins, single chain variable fragments (scFvs), enzymes, and antibodies to cells, antigens or pathogens, may be bound to any surface of the sensor. In an exemplary embodiment, receptors 5 cover as much of the sensor surface as possible. Preferably, receptors 5 cover the major faces of piezoelectric layer 7 and an optional non-piezoelectric layer 6. For example, when trying to detect cancer, monomeric and dimeric anti-tumor scFv molecules, which are composed of variable light and heavy chains of antibody molecule anti-ECD scFV that react to cancer markers, may be employed. Similarly, when trying to detect Bacillus anthracia (“BA”), antibodies specific to BA spore surface antigens may be employed.

Any means of adhering receptors 5 to a sensor surface may be utilized. In a preferred embodiment, receptors 5 may be bound to a surface of the sensor using an immobilization layer 4, such as self assembled monolayers (“SAM”), mercaptopropylsilane (MPS) and bi-functional linkers. In one exemplary embodiment, for purposes of binding scFv, the immobilization coating may be a self assembled monolayer of 3-mercaptoproprionic acid (MPA) on a copper, platinum, or gold-coated electrode activated with 1-ethyl-3-(3-dimethylaminopropy)carbodimide hydrochloride (EDC) and 5 mg/ml N-hydroxysulfosuccinimide (NHS).

In one embodiment, the piezoelectric microcantilever includes a highly piezoelectric layer 7, which enables electrical detection and actuation within the cantilever. The piezoelectric layer may function as a driving element, vibrating element, sensing element, or a combination thereof. Preferably, piezoelectric layer 7 is a driving, vibrating and sensing element. Applying an AC voltage (input) across piezoelectric layer 7 bends and vibrates the PEMS, which in turn induces a piezoelectric voltage that produces readily detectable changes in the magnitude and phase of the output voltage. The resonance frequency of the PEMS may be obtained, for example, by monitoring the maximum of the phase shift of the output voltage. This measurement is accomplished all-electrically, i.e., electrical actuation and electrical sensing.

Piezoelectric layer 7 may be constructed from any piezoelectric material, preferably highly piezoelectric materials, such as lead magnesium niobate-lead titanate (Pb(Mg_(1/3)Nb_(2/3))O₃)_(1-x)—(PbTiO₃)_(x) (PMN_(1-x)-PT_(x)) films (PMN-PT), where 0.3<x<0.4, highly piezoelectric lead zirconate titanate (PZT) films and sodium potassium niobate-lithium niobate solid solutions (NKN-LN). In an exemplary embodiment, piezoelectric layer 7 may be fabricated from any highly piezoelectric material with a high −d₃₁ coefficient of about 20 pm/V<−d₃₁<5000 pm/V, preferably about 200 pm/V<−d₃₁<5000 pm/V, more preferably, about 500 pm/V<−d₃₁<5000 pm/V and most preferably, about 2000 pm/V<−d₃₁<5000 pm/V. In another exemplary embodiment, the −d₃₁ coefficient may be greater than about 20×10⁻¹² mN. Additionally, piezoelectric layer 7 may have a piezoelectric coefficient d₃₃ greater than about 40×10⁻¹² m/V.

Piezoelectric layer 7 may have any structural configuration or dimension. In one exemplary embodiment, piezoelectric layer 7 may be rectangular, triangular, circular, elliptical, or any other geometric shape. In another exemplary embodiment, the piezoelectric layer has a thicknesses of about 0.5 μm to about 250 μm, more preferably about 0.5 μm to about 127 μm and most preferably about 0.5 μm to about 100 μm. Piezoelectric layer 7 may further have a length of about 1 μm to about 3 mm and a width of about 1 μm to about 3 mm. In yet another exemplary embodiment, piezoelectric layer 7 may further have a length of about 10 μm to about 3 mm and a width of about 0.5 μm to about 3 mm.

Optionally, the PEMS may also include at least one non-piezoelectric layer 6, which may be fabricated from any compatible material, including ceramic, polymeric, plastic, metallic material or a combination thereof. In an exemplary embodiment, non-piezoelectric layer 6 may be fabricated from silicon dioxide (SiO₂) or silicon nitride (Si₃N₄) for PZT-thin film based PEMS. In another exemplary embodiment, non-piezoelectric layer 6 may be fabricated from a metal such as Cu, Sn, Ni, Ti, or any combination thereof. Non-piezoelectric layer 6 may also have any structural configuration or dimension. In one exemplary embodiment, non-piezoelectric layer 6 may be rectangular, triangular, circular, elliptical, or any other geometric shape. In another exemplary embodiment, non-piezoelectric layer 6 may have a length of 1 μm to about 3 mm, a width of about 1 μm to about 3 mm and a thickness of about 0.05 μm to about 100 μm.

The piezoelectric microcantilever of the present invention includes a piezoelectric layer 7. In another exemplary embodiment, the PEMS may include a piezoelectric layer 7 and optionally, at least one non-piezoelectric layer 6. Piezoelectric layer 7 and/or optional non-piezoelectric layer 6 may be attached to a clamp. The microcantilever may have a wide variety of structural configurations. In one exemplary embodiment, a piezoelectric layer 7 may be bonded to a non-piezoelectric layer 6 that is shorter, longer or equal in length. Preferably, non-piezoelectric layer 6 may be shorter than or extend beyond piezoelectric layer 7, so as to form a cantilever tip. When flexural modes are not used, the preferred PEMS need not have a non-piezoelectric layer 6 so as to maximize the length-mode or width-mode resonance frequency shift. In yet another exemplary embodiment, a piezoelectric layer 7 may be wider than, narrower than or equal in one or more dimensions with respect to non-piezoelectric layer 6.

For applications involving detection in a liquid, the PEMS may further include an electrically insulating layer 3 in order to electrically separate or buffer conductive element 1 and second conductive element 2, thereby maintaining functionality by preventing conduction. Conductive element 1 may be patterned slightly smaller than the piezoelectric layer 7 to ensure complete insulation of the edges and corners thereof. Any electrically insulating layer 3 may be used as a coating to achieve electrical separation or buffering.

In one embodiment, insulating layer 3 may comprise a 1.5 μm thick parylene (poly-para-xylylene) coating deposited on a conductive element 1, 2 by chemical vapor deposition. When placed in static and 1 ml/min flow rate of PBS solution, a parylene insulating layer 3 essentially prevents background resonance frequency shifts greater than 30 Hz and 60 Hz, respectively, over a period of 30 minutes. As a result, insulating layer 3 enables complete submersion of the microcantilever for in situ or in-liquid detection while maintaining a Q value (quality value) greater than about 35.

Alternatively, a PEMS may be insulated using self-assembled monolayers with hydrophobic properties, preferably methyltrimethoxysilane (MTMS) or a combination of MTMS with parylene coatings of varying thicknesses, may also be used. When immersed in a PBS solution, an MTMS insulated piezoelectric microcantilever yields strong resonance peak intensities and prevents background resonance frequency shifts greater than about 30 Hz over a period of 30 minutes.

Other insulation materials may include Al₂O₃, SiO₂ and any functional hydrophobic silane, having a hydrophobic group selected from the group consisting of alkyl, phenyl, alkyl halide, alkene, alkyne, and sulfhydryl. In an exemplary embodiment, the insulation material is mercaptopropylsilane (MPTS), which can also function to immobilize a receptor on the cantilever.

The resultant PEMS may be chemically inert, thermally stable and preferably miniaturized to enhance sensitivity. In an exemplary embodiment, the PEMS has a high detection sensitivity of about 1×10⁻¹¹ g/Hz or better, more preferably 1×10⁻¹⁶ g/Hz or better and most preferably 1×10⁻¹⁷ g/Hz or better. Preferably, the PEMS has a detection sensitivity of about 1×10⁻¹⁹ g/Hz or better. Preferably, the PEMS may be electrically insulated to enable detection in any sample medium, including air, liquid or solid.

In operation, an alternating voltage may be applied to conductive element 1 to drive piezoelectric layer 7 of the self-actuating PEMS and a conductive element 2 may be used to detect a shift in the mechanical resonance frequency of the PEMS due to the binding of a target molecule or compound by the receptors. During this process, the method of the present invention involves inducing a positive or negative change in the Young's modulus of the piezoelectric layer, which is preferably a substantial change in the Young's modulus of the piezoelectric layer. In one exemplary embodiment, the change in the Young's modulus may be up to about 70%. The change in the Young's modulus of the piezoelectric layer is preferably greater than about 25%. Most preferably, the change in the Young's modulus may be about 25% to about 70%. One of the factors that induces a change in the Young's modulus is non-180° polarization domain switching.

By inducing and/or enhancing non-180° polarization domain switching, it may be possible to further increase the detection sensitivity of the PEMS in comparison to non-piezoelectric or weak piezoelectric microcantilevers of the same dimension. One means for inducing non-180° polarization domain switching may be application of stress produced by the binding of target molecules or compounds. In another exemplary embodiment, non-180° polarization domain switching may be induced by exposing the PEMS to a DC bias electric field. The DC bias electric field may be established using any conventional means and may involve applying a DC voltage across a thickness, length or width of piezoelectric layer 7. Preferably, the established DC bias electric field (E) is from about −20 kV/cm to about 20 kV/cm, more preferably, from about −10 kV/cm to about 10 kV/cm, and, most preferably, from about −8 kV/cm to about 10 kV/cm. A positive value for E denotes an applied electric field that is parallel to the poling direction of the piezoelectric layer. A negative value for E denotes an applied electric field that is opposite to the poling direction of the piezoelectric layer. By establishing a DC bias electric field, the flexural frequency shift and hence, detection sensitivity, may be further increased by a factor of up to about three in comparison to the sensitivity PEMS operated without a DC bias electric field. The DC bias electric field changes the polarization configuration such that it increases polarization domain switching, which in turn enhances the resonance frequency shift enabling enhanced detection sensitivity. The degree of detection sensitivity enhancement is dependent upon the piezoelectric material, the thickness of the piezoelectric layer, whether it is bonded to a non-piezoelectric layer, the physical properties, i.e. thickness and/or material characteristics of the non-piezoelectric layer and any combination thereof.

The method may further involve enabling detection of a species of interest using any resonance frequency peak and any resonance frequency modes. In an exemplary embodiment, the PEMS may be operated in a flexural resonance mode, a longitudinal resonance mode, such as a length mode, a width mode and/or a thickness mode, or a combination thereof. Preferably, the PEMS may be capable of length-mode and width-mode detection, which enables more sensitive detection with high peak frequency intensities and minimized damping effects. More preferably, the PEMS is capable of enhanced detection sensitivity using both flexural and longitudinal resonance modes. In an exemplary embodiment, the PEMS may be used at resonance frequencies within the range of about 10 kHz to about 10 GHz.

Additionally, to further increase sensitivity and expedite the detection process, the PEMS may be immersed in a flowing solution for in-liquid detection. The PEMS is preferably situated in a flow cell system to enable tailored, rapid and simultaneous detection and quantification of multiple organic compounds or molecules.

FIG. 2( a) shows a flow cell system 10, with a PEMS holder/measuring unit 11, having a total volume of about 0.03 ml to 10 ml, pump 12, and a mechanism for controlling temperature and humidity (not shown). The flow cell 10 may attain flow rates of 0.01-100 ml/min. The total volume of the flow cell, number of channels and flow rate may vary depending upon the number of compounds to be measured. The flow cell 10 may cooperate with a portable PEMS unit, shown in FIG. 2( b), which has multiple channels for the simultaneous quantification of multiple receptor specific molecules. The portable PEMS is inexpensive and capable of obtaining quick measurements.

These PEMS may be used for various sensing applications such as solid-liquid transition detectors, liquid viscosity and density sensors, mass sensors for in situ and in-water detection. The PEMS may generally be used to detect molecules, compounds, biological elements such as DNA, proteins, viruses, cells, spores, and parasites, or combinations thereof.

The PEMS technology may be particularly useful for the detection of bioterrorism agents. Antibody receptors specific to at least one bioterrorism agent may be bound to an electrode and used to detect the presence of a bioterrorism antigen. In addition to identifying the existence of a bioterrorism agent, it may also be used to quantify the concentration of the agent.

Additionally, PEMS may be useful in the health sciences as a diagnostic instrument. It may be used as a means for early detection of cancers and other diseases. It may also be used to monitor the progress of the disease throughout treatment. The PEMS may be incorporated in a portable device and used as a noninvasive means for testing blood and other bodily fluids for various pathogens, infectious agents and other markers indicative of disease.

PEMS may also be particularly applicable for the food science and food manufacturing industry. PEMS may be used as a diagnostic instrument for detecting pathogens or other disease agents present in food supplies and prepared or processed foods. Additionally, it may also be useful in manufacturing plants and food service industries as a means of intermittently checking food products during different phases of food preparations thereby preventing contamination and the spread of bacterial or viral diseases such as salmonella and E. coli.

EXAMPLES Example 1

The effect of a DC bias electric field on the flexural mode resonance frequency shift of a PMN-PT/tin PEMS, having a length of 650±100 μm, a width of 600±50 μm thickness of 14 μm, was investigated for humidity detection. The PEMS was constructed from an 8 μm PMN-PT freestanding film bonded to a 6-μm tin layer by electroplating. Alternatively, the non-piezoelectric layer may be fabricated from copper. A 30 nm thick nickel electrode with a 15 nm thick chromium bonding layer was deposited on one side of the PMN-PT freestanding film by E-beam evaporation (Semicore Equipment, Livermore, Calif.). The tin layer was subsequently electroplated on the nickel electrode and a 150 nm thick gold top electrode was deposited on the other side of the PMN-PT film by evaporation. The PMN-PT/Sn bilayer was then cut and configured as a rectangular strip with a wire saw (Princeton Scientific Precision, Princeton, N.J.). 25-μm thick gold wires (Kulicke & Soffa, Willow Grove, Pa.) were attached to the top and bottom electrodes using conductive glue (XCE 3104XL, Emerson and Cuming Company, Billerica, Mass.). The PMN-PT/Sn strip was then glued to a glass substrate to form a microcantilever, and the PEMS was subsequently subjected to poling at 20 kV/cm and a temperature of 120° C. on a hotplate for 30 minutes. FIG. 3( a) shows an optical micrograph of the fabricated PEMS and top gold electrode.

The performance of the PEMS was first measured without a DC bias electric field at a constant humidity. Subsequently, a DC bias electric field and changes in the relative humidity (RH) were applied to the PEMS system as means to induce stress and change the Young's modulus of the PEMS. The flexural-mode and width-mode resonance frequencies and dielectric constants of the PEMS were measured at different DC bias electric field strengths and at different relative humidity levels. Specifically, examples were carried out under a DC bias electric field varying from about −9 kV/cm to about 9 kV/cm and under relative humidity's of from 60% RH to 30% RH.

FIG. 3( b) shows the characteristics and performance of the PEMS measured in the absence of a DC bias electric field. Specifically, FIG. 3( b) shows the phase angle versus frequency resonance spectrum of the PEMS obtained by an electric impedance analyzer (Agilent 4294A, Agilent, Palo Alto, Calif.). The phase angle, θ=tan⁻¹(Im(I)/Re(I)), represents the angle between the real part, Re(I), and the imaginary part, Im(I), of the complex electrical impedance, I. Off resonance, the PEMS behaved as a capacitor with a phase angle

≅−90°. At resonance, the large mechanical vibrations induced a large piezoelectric voltage in phase with the input voltage causing θ to deviate from −90°. With the known Young's modulus and density of PMN-PT (tin) of E_(p)=80 GPa and ρ_(p)=7.9 g/cm³ (E_(n)=50 GPa and ρ_(n)=7.3 or 9.0 g/cm³), respectively, the theoretical flexural-mode resonance frequencies of the PEMS were calculated and marked by the dashed vertical lines in FIG. 3( b). FIG. 3( b) shows that the PEMS exhibited two flexural frequencies below 120 kHz with Q=60, 100 for the flexural mode and width mode, respectively.

To measure the effects of relative humidity changes on the resonance frequency, the PEMS was placed in a sealed glove box to control relative humidity. A humidifier was then connected to the glove box to first raise the relative humidity (RH) inside the glove box to 90%. Dry air was then circulated in the glove box to establish the desired humidity level. Prior to measuring resonance frequency, the humidity level was allowed to stabilize for period of 5-10 minutes. Throughout the study, the temperature inside the glove box was maintained at 23±0.1° C.

As an example, FIG. 4( a) shows a graph of phase angle as a function of the resonance frequency spectra of the PEMS at 30%, 40%, 50% and 60% RH with a DC bias electric field of −4 kV/cm. The resonance frequency increased with a decreasing relative humidity due to desorption of water molecules from the sensor surface.

FIG. 4( b) shows a graph of relative resonance frequency shift (Δf/f) versus relative humidity with application of a DC bias electric field of −4, 0 and 4 kV/cm. For purposes of this study, relative frequency shift is defined as the difference in the resonance frequency at a given humidity level in comparison to the resonance frequency at 60% RH, divided by the resonance frequency at 60% RH. As can be seen, from 60% RH to 30% RH, the relative resonance frequency shift was about 0.25% with a DC bias electric field of E=0 and E=4 kV/cm and about 0.63% with E=−4 kV/cm, which is about 2.5 times the shift when compared to E=0 and E=4 kV/cm. The relative resonance frequency shift per relative humidity change at −4 kV/cm was also about 2.5 times that at E=0 and 4 kV/cm. This clearly indicates that the presence of a negative DC bias electric field of about −4 kV/cm significantly enhanced the detection sensitivity of the PEMS.

For purposes of comparison, the relative resonance frequency shift due to the mass change of the PEMS from desorption of water molecules was deduced using the PEMS mass change,

(Δƒ/ƒ)_(mass) =−Δm/2M  (Equation 1)

where Δm=(ΔΓ_(Sn)+Δδ_(Au))wL and M=(ρ_(p)t_(p)+ρ_(n)t_(n))wL. ΔΓ_(Sn) and Δδ_(Au), respectively, denote the water molecule adsorption density change on the tin surface and on the gold surface. w and L represent the width and length of the PEMS, respectively, and ρ_(p)=7.9 g/cm³ and t_(p)=8 μM (ρ_(n)=7.3 g/cm³ and t_(n)=6 μm) represent the density and thickness of the PMN-PT (tin) layer, respectively. Using two 10 MHz QCMs, one with two gold surfaces and the other with one tin surface and one gold surface, it was found that the mass density changed on the tin surface and on the gold surface from 60% RH to 30% RH, where ΔΓF_(Sn)=−1.3 and ΔΓ_(Au)=−0.4 ng/mm², respectively. The deduced relative resonance frequency shift, (Δƒ/ƒ)_(mass)=8×10⁻⁶, was more than 400 times too small to account for the observed resonance frequency shift of 2.5×10⁻³ at E=0 and 4 kV/cm field and more than 800 times smaller than frequency shift of 6.5×10⁻³ at E=−4 kV/cm as shown in FIG. 4( b). These differences show that adsorption of the species of interest changed the Young's modulus of the PMN-PT layer and that application of a negative DC bias electric field further enhanced the change in the Young's modulus providing even better detection sensitivity.

This phenomenon may be explained by comparing the PEMS resonance frequency measurements. In the absence of relative humidity change, both the flexural resonance frequency and the dielectric constant varied with application of a DC bias electric field. FIGS. 5( a) and 5(b) show the relative resonance frequency shift, Δƒ(E)/ƒ, and relative dielectric constant change, Δ∈(E)/∈ as a function of the applied DC bias electric field, E, respectively, where Δƒ(E)=ƒ(E)−ƒ, Δ∈(E)=∈(E)−∈ and ƒ and ƒ(E) (∈ and ∈(E)) are the resonance frequencies (dielectric constant) at E=0 an E≠0, respectively. The slope of Δƒ(E)/ƒ at E=−4 kV/cm was about 2.5 times that at E=0 and 4 kV/cm. In addition, Δ∈(E)/∈ was found to be negative for E>0 and positive when E<0. The fact that the dielectric constant decreased with application of an increasing positive DC bias electric field indicated that a positive DC bias electric field switched the polarization from an in-plane direction to the poling direction as schematically shown in I of FIG. 5( b).

The increase in the dielectric as a result of application of an increasingly negative DC bias electric field, indicates that application of a negative DC bias electric field switched the polarization from a vertical direction to an in-plane direction in this field range as schematically illustrated in II of FIG. 5( b). These results indicated that the increase in the in-plane polarization due to application of a negative DC bias electric field of about −4 kV/cm increased the “switchability” of the polarization domains, thereby enhancing the resonance frequency shift in the presence of a negative DC bias electric field. In contrast, a positive DC bias electric field decreased the switch-ability of polarization domains causing a DC bias electric field induced clamping effect.

Example 2

The detection sensitivity of the PEMS was also investigated under application of DC bias electric fields ranging from −9 kV/cm to 9 kV/cm. FIG. 10 shows the relative resonance frequency shift as a function of relative humidity under applied DC bias electric fields ranging from −9 to 9 kV/cm. As can be seen, for relative humidity changes from 60% RH to 30% RH, a DC bias electric field of −6 kV/cm showed the largest resonance frequency shift of any of the applied DC bias fields, including zero.

For comparison, FIG. 11 shows the resonance frequency shift from 60% RH to 30% RH versus the applied DC bias electric field. As shown in FIG. 11, a DC bias field of −6 kV/cm produced a relative resonance frequency shift of 0.75%, three times that of the zero DC bias electric field resonance frequency shift of 0.25%. Note that the 0.75% relative frequency shift with a DC bias electric field of −6 kV/cm was also 1200 times greater than what could be accounted for by mass change alone, (Δƒ/ƒ)_(mass)=8×10⁻⁶.

Example 3

The relationship between a change in Young's modulus and the flexural mode resonance frequency shift was investigated for humidity detection using a PMN-PT/tin PEMS, having a length of 900±100 μm, a width of 700±50 μm and a thickness of 8 μm. The PMN-PT/tin PEMS was constructed from a gold coated 8-μm thick PMN-PT layer bonded to a 6-μm tin layer by electroplating. The two dissimilar surfaces of the PEMS, gold and tin, caused bending during the humidity detection, which was used to quantify detection-induced strain. The PEMS of this example is shown in the insert of FIG. 6( a). To quantify the Young's modulus change in the PMN-PT layer, a separate PMN-PT strip having a length of 900±100 μm, a width of 700±50 μm and a thickness of 8 μm, wherein both sides of the PMN-PT strip are coated with gold, was also employed for humidity detection.

FIG. 6( a) shows the flexural resonance spectra of the PEMS at 20% and 70% relative humidity, as measured by an Agilent 4294A impedance analyzer (Palo Alto, Calif.). The phase angle, θ=tan⁻¹(Im(I)/Re(I)), represents the angle between the real part, Re(I), and the imaginary part, Im(I), of the complex electrical impedance, I. FIG. 6( a) shows that the resonance frequency increased with decreasing relative humidity due to desorption of adsorbed water molecules.

FIG. 6( b) shows the relative resonance frequency shift, (Δf/f)_(RH), as a function of relative humidity, where ƒ and Δƒ represent the resonance frequency at 60% RH and the difference in the resonance frequency at a given humidity level in comparison to the resonance frequency at 60% RH, respectively. The subscripts RH, DC and deduced, denote that Δf/f was a function of the changes in relative humidity, DC bias electric field.

From 60% RH to 30% RH, it was found that ΔΓ_(Sn)=−1.3 and ΔΓT_(Au)=−0.4 ng/mm², respectively. Therefore, (Δƒ/ƒ)_(mass)=8×10⁻⁶, which was 400 times too small to account for the observed resonance frequency shift of 2.5×10⁻³ from 60% RH to 30% RH, as shown in FIG. 6( b).

FIG. 6( b) further shows tip displacement as a function of relative humidity. In FIG. 6( b), a negative d_(RH) indicates that the PEMS bent towards the tin side of the PEMS. The PEMS axial tip displacement, d_(RH), was monitored in situ during analyte detection using a LC-2450 laser displacement meter with a 0.5 μm resolution (Keyence). Because ΔΓ_(Sn) was around three times ΔΓ_(Au), the PEMS bent when the relative humidity was changed. Based on the value of d_(RH), it was possible to discern that the average lateral strain, ∈_(ave), of the PMN-PT layer was about 4×10⁻⁵, which is about 80 times too small to account for the measured (Δf/f)_(RH) shown in FIG. 6( b). Therefore strain did not contribute to the observed enhanced resonance frequency shift.

In a separate study, DC bias electric fields of 1-4 kV/cm were applied to the PEMS while the resonance frequency shift, (Δƒ/ƒ)_(DC), and the tip displacement, d_(DC), were simultaneously measured, where ƒ and Δƒ represent the flexural resonance frequency at E=0 and the difference of the resonance at a given E in comparison to E=0, respectively. As shown in FIG. 6( b), an E>0 denotes an electric field parallel to the poling direction of the PMN-PT layer. For both (Δƒ/ƒ)_(DC) and d_(DC), the effect of decreasing the relative humidity from 60% RH to 30% RH was found to have a similar effect as that of changing E from 0 to 3 kV/cm. Without wishing to be bound by theory, since neither the mass loading effect nor the detection-induced strain accounts for the observed Δƒ/ƒ, the similarity between the effect of the change in humidity and the change in the DC bias electric field suggests that both changes in relative humidity and DC bias electric field may cause a change in the Young's modulus of the PMN-PT layer.

Example 4

To examine whether the Young's modulus of the PMN-PT layer changed during humidity detection, the width mode resonance frequency of a PMN-PT strip having cantilever geometry was investigated. To ensure that the lateral stress of the PMN-PT strip did not change signs across its thickness, the PMN-PT strip was coated with two identical gold surfaces, such that no bending occurred in the PMN-PT strip during humidity detection. Additionally, the PMN-PT strip did not include a non-piezoelectric layer; therefore, it did not exhibit a flexural-mode resonance peak. Insert I of FIG. 7 shows an optical micrograph of the PMN-PT strip and Insert II of FIG. 7 shows the first width-mode resonance spectra of the PMN-PT strip at 30% RH and 60% RH. As can be seen from the inserts in FIG. 7, the width-mode resonance frequency changed with the relative humidity.

FIG. 7 shows that the width mode resonance of the PMN-PT strip shifted with changing relative humidity levels. The increasing (Δƒ/ƒ)_(RH) with decreasing relative humidity indicated that the lateral Young's modulus of the strip changed as a result of changes in relative humidity. Furthermore, the PMN-PT width mode and flexural mode resonance frequencies appear to be similar since both the width mode and flexural mode resonance frequency shifts increased with decreasing relative humidity levels.

FIG. 7 also shows the width mode resonance frequency shift of the PMN-PT strip when subjected to a DC bias electric field. The resultant width mode resonance frequency shift shows that the effect of a positive E was similar to that of a decreasing relative humidity.

The width mode resonance frequency, ƒ_(w), is related to the lateral Young's modulus, Y_(p), as shown in Equation 2,

ƒ_(w)=(Y _(p)/ρ_(p))^(1/2)/2w,  (Equation 2)

where ρ_(p) and w represent the density and width the PMN-PT strip.

Because

$\frac{\Delta \; f_{w}}{f_{w}}{\operatorname{<<}1}$

and because the width change was negligible, the relative change in the Young's modulus may be expressed as Equation 3.

$\begin{matrix} {\left( \frac{\Delta \; Y_{P}}{Y_{P}} \right)_{strip} \cong {2\frac{\Delta \; f_{w}}{f_{w}}}} & \left( {{Equation}\mspace{14mu} 3} \right) \end{matrix}$

The relative Young's modulus change of the PMN-PT layer therefore was calculated according to Equation 5.

Without wishing to be bound by theory, the deduced change in the Young's modulus of the PMN-PT layer appears to validate that the Young's modulus change was the underlying mechanism for the PEMS flexural-mode resonance frequency shift during the humidity detection. As shown in FIG. 6( b), the deduced Δƒ/ƒ as a function of relative humidity overlapped with the experimental results. FIG. 8 further confirms that the flexural resonance frequency shift, which provides enhanced detection sensitivity, is induced by a change in the Young's modulus of the PMN-PT layer. FIG. 8 shows (Δf/f) as a function of average bending strain, −∈_(ave), at the outer surface of the PMN-PT layer, which is calculated from the axial tip displacement of FIG. 6( b). The relative resonance frequency shift correlated with the lateral strain regardless of whether the resonance frequency shift was caused by a DC bias electric field or by a change in humidity. Additionally, by comparing FIGS. 6 a-8, the change in the Young's modulus appears to be caused by non-180° polarization domain switching as polarization domain pattern changes were observed in piezoresponse force microscopy (PFM). A schematic of the polarization domain switching in a DC electric field is shown in FIG. 9. For comparison, the average stresses in the PMN-PT layer due to the adsorption or desorption of water molecules and due to application of a DC bias electric field were estimated as σ_(ave,RH)=Y_(p)∈_(ave,RH) and σ_(ave,DC)=Y_(p)∈_(ave,DC), respectively. FIG. 8 shows that both σ_(ave,RH) and σ_(ave,DC) were on the order of MPa and the relative Young's modulus change was about 0.5% per MPa stress in the PMN-PT layer, which was comparable to the 1-1.5% Young's modulus change per MPa stress reported for unpoled lead zirconate titanate (PZT). Without wishing to be bound by theory, it appears that the stress effect can induce much larger frequency shifts than predicted by mass loading in chemical and biological detection because surface stress causes a change in the Young's modulus, inducing a change in the spring constant of the PEMS. Furthermore, a change in the Young's modulus may be induced by non-180° polarization domain switching due to analyte binding and/or by application of a DC bias electric field.

It is to be understood, however, that even though numerous characteristics and advantages of the present invention have been set forth in the foregoing description, together with details of the structure and function of the invention, the disclosure is illustrative only, and changes may be made in detail, especially in matters of shape, size and arrangement of parts within the principles of the invention to the full extent indicated by the broad general meaning of the terms in which the appended claims are expressed. 

1. A method for using a piezoelectric microcantilever sensor comprising the steps of: inducing a change in the Young's modulus of a piezoelectric layer of the piezoelectric microcantilever sensor, and detecting a species of interest by measuring a frequency shift of said piezoelectric layer having a changed Young's modulus, wherein said frequency shift is caused by binding of said species of interest to receptors on said microcantilever sensor.
 2. A method as claimed in claim 1, wherein said change in the Young's modulus of the piezoelectric layer is induced by applying a DC bias electric field to said microcantilever sensor to cause non-180° polarization domain switching in said piezoelectric layer.
 3. The method claim 2, wherein the DC bias electric field is from about −20 kV/cm to about 20 kV/cm.
 4. The method claim 1, wherein the piezoelectric layer is selected from the group consisting of PZT, PMN-PT and NKN-LN.
 5. The method claim 1, wherein the piezoelectric layer has a thickness of from about 0.5 μm to about 250 μm.
 6. The method claim 1, wherein the piezoelectric layer has a thickness of from about 0.5 μm to about 127 μm.
 7. The method claim 1, wherein the piezoelectric layer has a thickness of from about 0.5 μm to about 100 μm.
 8. The method claim 1, wherein the piezoelectric layer has a piezoelectric coefficient −d₃₁ of about 20 pm/V to about 5000 pm/V.
 9. The method claim 1, wherein the piezoelectric layer has a piezoelectric coefficient −d₃₁ greater than about 20 pm/V.
 10. The method claim 1, wherein the piezoelectric layer has a piezoelectric coefficient d₃₃ greater than about 40 pm/V.
 11. The method claim 1, wherein the piezoelectric microcantilever sensor further comprises an electrical insulation layer which enables the sensor to substantially withstand liquid damping.
 12. The method claim 1, wherein the piezoelectric microcantilever sensor may further comprise a non-piezoelectric layer selected from the group consisting of: a metal, a ceramic and a plastic layer.
 13. The method claim 1, wherein during the detection step the piezoelectric microcantilever sensor is operated in a mode selected from the group consisting of: flexural mode and longitudinal mode.
 14. The method claim 13, wherein during the detection step, the piezoelectric microcantilever is operated in a longitudinal mode selected from the group consisting of: length mode, width mode or thickness mode.
 15. The method claim 1, wherein the DC bias electric field is from about −10 kV/cm to about 10 kV/cm.
 16. The method of claim 1, wherein said change in the Young's modulus is from about 25% to about 70%.
 17. The method of claim 16, wherein said change in the Young's modulus is induced by binding of the species of interest to receptors on said microcantilever sensor.
 18. A piezoelectric microcantilever sensor system comprising: a piezoelectric microcantilever sensor including a piezoelectric layer, at least one conducting element operatively associated with the piezoelectric layer and at least one receptor capable of binding a species of interest; and a DC bias electric field generation means associated with said piezoelectric microcantilever sensor for applying a DC bias electric field to said piezoelectric layer sufficient to cause non-180° polarization domain switching in said piezoelectric layer.
 19. The system of claim 18, wherein said DC bias electric field generation means enhances non-180° polarization domain switching of said piezoelectric layer by application of a DC bias electric field of from about −20 kV/cm to about 20 kV/cm.
 20. The method of claim 19, wherein application said DC bias electric field enhances the detection sensitivity of the piezoelectric microcantilever sensor. 